Exam 42: Energy From the Nucleus

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The first step of the proton-proton cycle is:

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Separation of the isotopes of uranium requires a physical, rather than chemical, method because:

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In the uranium disintegration series:

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Tokamaks confine deuteron plasmas using:

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Consider all possible fission events.Which of the following statements is true?

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The energy released in a complete proton-proton cycle is about:

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The overall proton-proton cycle is equivalent to:

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Nuclear fusion in stars produces all the chemical elements with mass numbers less than:

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Which one of the following represents a fission reaction that can be activated by slow neutrons?

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Two billion years ago, a natural nuclear reactor formed in a uranium deposit in Africa.Why is it not possible for such a natural reactor to form somewhere on Earth today?

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Lawson's number is 1020 s.m-3.If the density of deuteron nuclei is 2 * 1021 m-3 what should the confinement time be to achieve sustained fusion?

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For purposes of a practical (energy producing)reaction one wants a disintegration energy Q that is:

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In a subcritical nuclear reactor:

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The energy supplied by a thermal neutron in a fission event is essentially its:

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A nuclear reactor is operating at a certain power level, with its multiplication factor adjusted to unity.The control rods are now used to reduce the power output to one-half its former value.After the reduction in power the multiplication factor is maintained at:

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The table lists properties of several heavy nuclei when they are struck by thermal neutrons; En is the excitation energy and Eb is the energy barrier.Which quantity, or combination of quantities, represents the energy put into the oscillation of the resulting compound nucleus? The table lists properties of several heavy nuclei when they are struck by thermal neutrons; E<sub>n</sub> is the excitation energy and E<sub>b</sub> is the energy barrier.Which quantity, or combination of quantities, represents the energy put into the oscillation of the resulting compound nucleus?

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Most of the energy produced by the Sun is due to:

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235U is readily made fissionable by a thermal neutron but 238U is not because:

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When 236U fissions the fragments are:

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For a controlled nuclear fusion reaction, one needs:

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